Download citation
Download citation
link to html
In the title compound, [Pd(C6H5)(C10H11O2S)(C18H15P)]·C4H8O, an iso­propyl­thio­benzoate ligand is coordinated in a bidentate fashion to the central Pd atom through the O and S atoms. The square-planar geometry of the Pd atom is completed by a phenyl ligand and a tri­phenyl­phosphine group but is distorted by the bidentate ligand, which forms a six-membered chelate ring. This ring deviates strongly from planarity, which is illustrated by the plane through the phenyl portion of the chelate ring forming a dihedral angle of 62.3 (1)° with the coordination plane.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270199016480/fr1232sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270199016480/fr1232Isup2.hkl
Contains datablock I

CCDC reference: 143243

Comment top

The title compound, (I), was synthesized for its potential catalytic properties in C—C linkage reactions, such as the oligomerization of ethene. P—O hemilabile ligands coordinated to Ni are well known in such reactions, and the catalytic mechanism proposed by Rauchfuss et al. (1975) can also be applied to S—O hemilabile ligands. The hemilabile ligand may be either monodentate (coordinated only through the O) or bidentate (coordinated through both S and O). In the presence of a substrate molecule the S of the complex containing the bidentate ligand will decoordinate leaving a vacant coordination site. Since the hemilabile ligand is still bound to the Pd through the O, the S atom is close enough to recoordinate to the Pd once the catalytic reaction has taken place. \scheme

The synthesis and characterization of a series of Pd complexes containing potentially hemilabile S—O ligands, of the type trans-[Pd(OOC-C6H4-2-SR-κO)(C6H5){P(C6H5)3}2], have previously been reported [R = Et was described by Meyer et al., (1998), while the two conformational isomers of R = Me were discussed by Kruger et al. (2000)]. Although the hemilability of the complexes has been proven in solution, all the previously reported crystal structures were of the monodentate form. This paper presents the first example of a crystal structure of a Pd complex with bidentate coordination of the S—O ligand, through both the S and O atoms.

The molecular structure and atom-numbering scheme for (I) are shown in Fig. 1. The majority of the bond lengths and angles agree with those found in the previously determined ethylthiobenzoate and methylthiobenzoate structures, although the Pd—P bond length of 2.279 (1) Å is shorter. This suggests that the trans influence of the S is smaller than that of P (the trans ligand in the previously determined structures).

The conformation of the chelate ring agrees with the findings of Corey & Bailar (1959). They determined that enhanced puckering of a six-membered ring occurred when a metal-N bond distance was greater than 2 Å and the bite-angle of the chelate was close to 90°. This increased the interactions of cis substituents, thus destabilizing the ring, particularly when bulky substituents were present. This is clearly the case in the present structure, where the bond angle is close to 90° and the chelate ring is extremely buckled, whereas the previous monodentate methylthiobenzoate and ethylthiobenzoate ligands were planar. The extent of the puckering is illustrated by the phenyl portion of the ligand (C42—C47), which is tilted at an angle of 62.3 (1)° to the molecular plane containing the Pd, and by the deviations from 0 or 180° in the torsion angles shown in Table 1.

Although the bond angles around the Pd do not deviate substantially from the expected 90 and 180°, the planarity of the square-planar conformation around the Pd is affected by the puckered ligand, giving a tetrahedral distortion. A calculation of the best plane through the Pd and the four atoms bonded to it showed that the Pd lies only 0.009 (1) Å above the plane, whereas the trans C31 and O41 lie 0.173 (2) and 0.180 (2) Å, respectively, above the plane and the P and S lie 0.182 (1) and 0.181 (1) Å, respectively, below the plane.

Experimental top

Thallium 2-isopropylthiobenzoate was obtained by stirring thallium carbonate with the stoichiometric amount of 2-isopropylthiobenzoic acid in methanol at ca 313 K for 30 min and removing the solvent in vacuo. The salt was then added in 20% excess to a solution of [Pd(tmeda)(C6H5)I] (tmeda = tetramethylethylenediamine) in tetrahydrofuran (THF) and the mixture stirred for 1 h at room temperature. A solution of the stoichiometric amount of triphenylphosphine in THF was added dropwise to the suspension over a period of 1 h. After stirring overnight the precipitated thallium iodide was removed by filtration through Celite. The volume of the solution was reduced to one third and layered with n-pentane. Single crystals of (I) were obtained at room temperature in a yield of 30% with no further crystallization.

Refinement top

The THF molecule was found to be disordered. This was resolved by a rigid body refinement of an ideal molecule, which showed that the disorder could be described by three different conformations in the ratio 40:27:33. Each conformation was refined with common isotropic displacement parameters.

Computing details top

Data collection: SMART (Siemens, 1996); data reduction: SAINT (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEX (McArdle, 1995); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular conformation of (I) showing the atom-numbering scheme and the disordered solvent. Displacement ellipsoids are shown at the 50% probability level and H atoms are drawn as spheres of arbitrary radii.
[(2-isopropylthio)benzoato-O,S]phenyl(triphenylphosphine)palladium(II) tetrahydrofuran solvate top
Crystal data top
[Pd(C10H11O2S)(C6H5)(C18H15P)]·C4H8OZ = 2
Mr = 713.12F(000) = 736
Triclinic, P1Dx = 1.369 Mg m3
a = 9.8574 (6) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.9503 (6) ÅCell parameters from 7829 reflections
c = 16.5057 (10) Åθ = 1.3–25.0°
α = 100.142 (1)°µ = 0.68 mm1
β = 95.803 (1)°T = 293 K
γ = 96.244 (1)°Prism, colourless
V = 1730.2 (2) Å30.30 × 0.25 × 0.20 mm
Data collection top
Siemens SMART CCD area detector
diffractometer
5613 independent reflections
Radiation source: fine-focus sealed tube5028 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
ω scansθmax = 25.0°, θmin = 1.3°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 1111
Tmin = 0.82, Tmax = 0.87k = 1013
7829 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: patterson
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.097H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0318P)2 + 2.4317P]
where P = (Fo2 + 2Fc2)/3
5613 reflections(Δ/σ)max = 0.019
386 parametersΔρmax = 0.66 e Å3
1 restraintΔρmin = 0.50 e Å3
Crystal data top
[Pd(C10H11O2S)(C6H5)(C18H15P)]·C4H8Oγ = 96.244 (1)°
Mr = 713.12V = 1730.2 (2) Å3
Triclinic, P1Z = 2
a = 9.8574 (6) ÅMo Kα radiation
b = 10.9503 (6) ŵ = 0.68 mm1
c = 16.5057 (10) ÅT = 293 K
α = 100.142 (1)°0.30 × 0.25 × 0.20 mm
β = 95.803 (1)°
Data collection top
Siemens SMART CCD area detector
diffractometer
5613 independent reflections
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
5028 reflections with I > 2σ(I)
Tmin = 0.82, Tmax = 0.87Rint = 0.017
7829 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0411 restraint
wR(F2) = 0.097H-atom parameters constrained
S = 1.10Δρmax = 0.66 e Å3
5613 reflectionsΔρmin = 0.50 e Å3
386 parameters
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Equation of least-squares plane through Pd, C31, O41, S and P: - 5.9973 (0.0075) x + 9.3474 (0.0050) y - 2.2261 (0.0168) z = 1.7945(0.0061) Deviations of atoms from least-squares plane (* indicates included in calculation) * 0.0093 (0.0011) Pd * 0.1802 (0.0016) C31 * 0.1732 (0.0015) O41 * -0.1817 (0.0011) S * -0.1810 (0.0011) P

Rms deviation of fitted atoms = 0.1602

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement.

The structure was solved by interpretation of a Patterson synthesis which yielded the position of the metal atom, while the remaining non-metal atoms were found from the difference Fourier maps. The H atoms could be located by difference Fourier, but were refined in ideal positions with bond lengths of 0.93 Å for aromatic C—H bonds, 0.98 Å for the tertiary C—H bond and 0.96 Å for the rest, and with displacement parameters 1.2 times that of the atom on which they were riding.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Pd0.60081 (3)0.75046 (3)0.722268 (17)0.03841 (10)
P0.76178 (9)0.85819 (8)0.82645 (6)0.0360 (2)
S0.45320 (11)0.61017 (9)0.61663 (6)0.0473 (2)
O410.4665 (3)0.7017 (2)0.80562 (16)0.0495 (7)
O420.3153 (4)0.5801 (3)0.8552 (2)0.0755 (10)
C410.4007 (4)0.5951 (4)0.8078 (2)0.0480 (10)
C420.4270 (4)0.4801 (4)0.7481 (2)0.0483 (10)
C430.4295 (5)0.3691 (4)0.7782 (3)0.0632 (12)
H430.41850.36960.83360.076*
C440.4475 (6)0.2592 (4)0.7289 (4)0.0772 (15)
H440.45230.18740.75120.093*
C450.4586 (6)0.2553 (4)0.6461 (3)0.0753 (14)
H450.46820.18020.61220.090*
C460.4555 (5)0.3627 (4)0.6132 (3)0.0625 (12)
H460.46160.35980.55710.075*
C470.4432 (4)0.4755 (3)0.6646 (2)0.0454 (9)
C510.2805 (5)0.6577 (4)0.6177 (3)0.0581 (11)
H510.25860.67490.67490.057 (12)*
C520.2845 (6)0.7765 (5)0.5823 (4)0.0785 (15)
H5210.19680.80690.58360.095 (19)*
H5220.30470.75910.52600.084 (18)*
H5230.35440.83870.61470.078 (16)*
C530.1753 (6)0.5546 (6)0.5663 (5)0.098 (2)
H5310.18580.47720.58450.11 (2)*
H5320.18920.54600.50890.13 (3)*
H5330.08450.57540.57290.12 (2)*
C310.7046 (4)0.8153 (4)0.6382 (2)0.0469 (9)
C320.8022 (5)0.7541 (5)0.5991 (3)0.0614 (12)
H320.82670.68100.61450.074*
C330.8645 (6)0.8008 (7)0.5365 (3)0.0875 (18)
H330.93030.75880.51060.105*
C340.8292 (8)0.9077 (8)0.5133 (4)0.103 (2)
H340.87180.93930.47220.123*
C350.7314 (8)0.9686 (6)0.5504 (4)0.098 (2)
H350.70571.04020.53340.118*
C360.6702 (5)0.9238 (5)0.6133 (3)0.0702 (14)
H360.60540.96710.63910.084*
C1110.7117 (4)1.0047 (3)0.8766 (2)0.0407 (8)
C1120.8047 (5)1.1093 (4)0.9138 (3)0.0601 (12)
H1120.89791.10960.90900.072*
C1130.7581 (6)1.2125 (4)0.9579 (3)0.0755 (15)
H1130.82061.28200.98290.091*
C1140.6217 (7)1.2137 (5)0.9653 (3)0.0751 (15)
H1140.59141.28370.99510.090*
C1150.5297 (6)1.1117 (5)0.9288 (3)0.0765 (15)
H1150.43681.11230.93430.092*
C1160.5736 (5)1.0080 (4)0.8840 (3)0.0583 (11)
H1160.50990.93970.85850.070*
C1210.9402 (4)0.8938 (3)0.8071 (2)0.0417 (9)
C1221.0435 (4)0.8344 (4)0.8389 (3)0.0523 (10)
H1221.02300.77580.87180.063*
C1231.1779 (5)0.8606 (5)0.8227 (3)0.0699 (13)
H1231.24710.82020.84460.084*
C1241.2072 (5)0.9462 (5)0.7742 (3)0.0716 (14)
H1241.29720.96440.76330.086*
C1251.1057 (5)1.0061 (5)0.7413 (3)0.0676 (13)
H1251.12701.06410.70810.081*
C1260.9722 (4)0.9804 (4)0.7575 (3)0.0543 (10)
H1260.90351.02100.73520.065*
C1310.7733 (4)0.7668 (3)0.9089 (2)0.0400 (8)
C1320.8075 (4)0.8223 (4)0.9913 (2)0.0507 (10)
H1320.82560.90901.00640.061*
C1330.8148 (5)0.7488 (5)1.0513 (3)0.0660 (13)
H1330.83860.78661.10670.079*
C1340.7877 (5)0.6218 (5)1.0304 (3)0.0734 (14)
H1340.79270.57301.07110.088*
C1350.7530 (6)0.5669 (5)0.9488 (4)0.0790 (16)
H1350.73450.48020.93430.095*
C1360.7450 (5)0.6383 (4)0.8877 (3)0.0626 (12)
H1360.72060.59980.83240.075*
O611.0980 (15)0.6298 (16)0.3639 (8)0.152 (4)*0.402 (4)
C611.013 (2)0.6997 (15)0.3359 (10)0.152 (4)*0.402 (4)
H61A1.05690.78550.34390.183*0.402 (4)
H61B0.93230.69830.36460.183*0.402 (4)
C620.978 (2)0.6515 (18)0.2526 (12)0.152 (4)*0.402 (4)
H62A1.04090.68840.21950.183*0.402 (4)
H62B0.88490.66440.23410.183*0.402 (4)
C630.989 (2)0.5250 (18)0.2493 (12)0.152 (4)*0.402 (4)
H63A0.90590.48090.26280.183*0.402 (4)
H63B1.00800.48540.19500.183*0.402 (4)
C641.0985 (18)0.5293 (17)0.3089 (11)0.152 (4)*0.402 (4)
H64A1.08880.45590.33420.183*0.402 (4)
H64B1.18400.53240.28450.183*0.402 (4)
O621.1878 (18)0.6391 (17)0.2557 (12)0.133 (6)*0.272 (9)
C651.057 (2)0.612 (2)0.2115 (13)0.133 (6)*0.272 (9)
H65A1.03900.52410.18560.159*0.272 (9)
H65B1.04850.66170.16850.159*0.272 (9)
C660.959 (3)0.642 (2)0.2716 (15)0.133 (6)*0.272 (9)
H66A0.93060.57080.29630.159*0.272 (9)
H66B0.87780.67020.24590.159*0.272 (9)
C671.042 (3)0.745 (2)0.3342 (14)0.133 (6)*0.272 (9)
H67A1.03980.82550.31720.159*0.272 (9)
H67B1.01030.75010.38830.159*0.272 (9)
C681.181 (2)0.706 (2)0.3347 (13)0.133 (6)*0.272 (9)
H68A1.25050.77910.34770.159*0.272 (9)
H68B1.19600.65460.37600.159*0.272 (9)
O631.1887 (17)0.6006 (18)0.3255 (10)0.143 (5)*0.325 (9)
C691.122 (2)0.5059 (18)0.2695 (13)0.143 (5)*0.325 (9)
H69A1.08710.43870.29620.171*0.325 (9)
H69B1.18200.47380.23030.171*0.325 (9)
C6101.012 (2)0.553 (2)0.2287 (14)0.143 (5)*0.325 (9)
H61C0.93040.54510.25660.171*0.325 (9)
H61D0.99030.50970.17140.171*0.325 (9)
C6111.066 (2)0.6800 (19)0.2342 (15)0.143 (5)*0.325 (9)
H61E1.12230.69010.19030.171*0.325 (9)
H61F0.99340.73280.23220.171*0.325 (9)
C6121.146 (2)0.7068 (17)0.3123 (12)0.143 (5)*0.325 (9)
H61G1.22360.76940.31290.171*0.325 (9)
H61H1.09100.73830.35510.171*0.325 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pd0.04090 (17)0.03779 (16)0.03584 (17)0.00140 (11)0.00478 (12)0.00903 (11)
P0.0375 (5)0.0325 (5)0.0381 (5)0.0026 (4)0.0036 (4)0.0090 (4)
S0.0558 (6)0.0485 (5)0.0346 (5)0.0055 (4)0.0045 (4)0.0080 (4)
O410.0567 (17)0.0472 (15)0.0424 (15)0.0061 (13)0.0150 (13)0.0048 (12)
O420.100 (3)0.063 (2)0.067 (2)0.0080 (18)0.046 (2)0.0140 (16)
C410.058 (3)0.048 (2)0.039 (2)0.0006 (19)0.009 (2)0.0133 (17)
C420.050 (2)0.048 (2)0.046 (2)0.0046 (18)0.0065 (19)0.0135 (18)
C430.076 (3)0.058 (3)0.060 (3)0.003 (2)0.013 (2)0.023 (2)
C440.101 (4)0.049 (3)0.084 (4)0.009 (3)0.013 (3)0.021 (3)
C450.094 (4)0.044 (3)0.084 (4)0.013 (2)0.009 (3)0.001 (2)
C460.074 (3)0.056 (3)0.054 (3)0.004 (2)0.007 (2)0.003 (2)
C470.048 (2)0.043 (2)0.044 (2)0.0010 (17)0.0029 (18)0.0085 (17)
C510.056 (3)0.063 (3)0.054 (3)0.002 (2)0.005 (2)0.017 (2)
C520.084 (4)0.070 (3)0.084 (4)0.012 (3)0.003 (3)0.029 (3)
C530.076 (4)0.087 (4)0.115 (6)0.014 (3)0.033 (4)0.021 (4)
C310.047 (2)0.049 (2)0.043 (2)0.0052 (18)0.0023 (19)0.0143 (17)
C320.058 (3)0.076 (3)0.047 (3)0.005 (2)0.013 (2)0.008 (2)
C330.068 (3)0.129 (5)0.057 (3)0.022 (3)0.023 (3)0.004 (3)
C340.102 (5)0.136 (6)0.066 (4)0.047 (5)0.005 (4)0.049 (4)
C350.106 (5)0.099 (5)0.095 (5)0.021 (4)0.000 (4)0.065 (4)
C360.075 (3)0.067 (3)0.076 (3)0.002 (2)0.009 (3)0.039 (3)
C1110.045 (2)0.0357 (19)0.043 (2)0.0073 (16)0.0032 (17)0.0097 (16)
C1120.057 (3)0.043 (2)0.076 (3)0.0032 (19)0.003 (2)0.006 (2)
C1130.100 (4)0.039 (2)0.078 (3)0.007 (2)0.015 (3)0.001 (2)
C1140.115 (5)0.053 (3)0.063 (3)0.034 (3)0.019 (3)0.006 (2)
C1150.077 (4)0.068 (3)0.092 (4)0.029 (3)0.031 (3)0.009 (3)
C1160.056 (3)0.054 (2)0.064 (3)0.009 (2)0.009 (2)0.006 (2)
C1210.039 (2)0.041 (2)0.043 (2)0.0001 (16)0.0040 (17)0.0044 (16)
C1220.045 (2)0.056 (2)0.058 (3)0.0128 (19)0.008 (2)0.014 (2)
C1230.045 (3)0.084 (3)0.084 (4)0.020 (2)0.012 (2)0.015 (3)
C1240.049 (3)0.090 (4)0.074 (3)0.003 (3)0.019 (3)0.013 (3)
C1250.061 (3)0.073 (3)0.064 (3)0.017 (2)0.010 (2)0.016 (2)
C1260.044 (2)0.058 (3)0.062 (3)0.0015 (19)0.004 (2)0.019 (2)
C1310.0350 (19)0.043 (2)0.045 (2)0.0038 (15)0.0067 (16)0.0159 (16)
C1320.054 (2)0.052 (2)0.047 (2)0.0049 (19)0.007 (2)0.0128 (18)
C1330.071 (3)0.090 (4)0.044 (2)0.016 (3)0.009 (2)0.025 (2)
C1340.080 (4)0.081 (4)0.074 (4)0.012 (3)0.017 (3)0.052 (3)
C1350.099 (4)0.050 (3)0.093 (4)0.002 (3)0.000 (3)0.035 (3)
C1360.085 (3)0.040 (2)0.061 (3)0.005 (2)0.004 (2)0.013 (2)
Geometric parameters (Å, º) top
Pd—C311.988 (4)C123—C1241.362 (7)
Pd—O412.098 (3)C123—H1230.9300
Pd—P2.2788 (10)C124—C1251.373 (7)
Pd—S2.3611 (10)C124—H1240.9300
P—C1311.828 (4)C125—C1261.378 (6)
P—C1111.814 (4)C125—H1250.9300
P—C1211.831 (4)C126—H1260.9300
S—C471.791 (4)C131—C1361.379 (5)
S—C511.835 (5)C131—C1321.380 (5)
O41—C411.281 (5)C132—C1331.383 (6)
O42—C411.223 (5)C132—H1320.9300
C41—C421.519 (6)C133—C1341.363 (7)
C42—C471.397 (5)C133—H1330.9300
C42—C431.394 (6)C134—C1351.367 (7)
C43—C441.369 (7)C134—H1340.9300
C43—H430.9300C135—C1361.383 (6)
C44—C451.374 (7)C135—H1350.9300
C44—H440.9300C136—H1360.9300
C45—C461.381 (6)O61—C611.297 (12)
C45—H450.9300O61—C641.298 (12)
C46—C471.393 (6)C61—C621.377 (13)
C46—H460.9300C61—H61A0.9700
C51—C531.516 (7)C61—H61B0.9700
C51—C521.516 (6)C62—C631.393 (13)
C51—H510.9800C62—H62A0.9700
C52—H5210.9600C62—H62B0.9700
C52—H5220.9600C63—C641.377 (13)
C52—H5230.9600C63—H63A0.9700
C53—H5310.9600C63—H63B0.9700
C53—H5320.9600C64—H64A0.9700
C53—H5330.9600C64—H64B0.9700
C31—C321.381 (6)O62—C651.392 (17)
C31—C361.388 (6)O62—C681.392 (17)
C32—C331.397 (7)C65—C661.477 (18)
C32—H320.9300C65—H65A0.9700
C33—C341.363 (9)C65—H65B0.9700
C33—H330.9300C66—C671.495 (18)
C34—C351.365 (10)C66—H66A0.9700
C34—H340.9300C66—H66B0.9700
C35—C361.387 (7)C67—C681.477 (18)
C35—H350.9300C67—H67A0.9700
C36—H360.9300C67—H67B0.9700
C111—C1161.382 (6)C68—H68A0.9700
C111—C1121.393 (5)C68—H68B0.9700
C112—C1131.381 (6)O63—C6121.325 (15)
C112—H1120.9300O63—C691.325 (15)
C113—C1141.364 (8)C69—C6101.405 (16)
C113—H1130.9300C69—H69A0.9700
C114—C1151.365 (7)C69—H69B0.9700
C114—H1140.9300C610—C6111.423 (16)
C115—C1161.379 (6)C610—H61C0.9700
C115—H1150.9300C610—H61D0.9700
C116—H1160.9300C611—C6121.406 (16)
C121—C1221.375 (5)C611—H61E0.9700
C121—C1261.390 (5)C611—H61F0.9700
C122—C1231.387 (6)C612—H61G0.9700
C122—H1220.9300C612—H61H0.9700
C31—Pd—O41170.24 (14)C123—C124—H124119.6
C31—Pd—P90.77 (11)C125—C124—H124119.6
O41—Pd—P92.60 (8)C124—C125—C126120.0 (5)
C31—Pd—S90.71 (11)C124—C125—H125120.0
O41—Pd—S87.47 (8)C126—C125—H125120.0
P—Pd—S170.55 (4)C125—C126—C121120.0 (4)
C131—P—C111103.81 (17)C125—C126—H126120.0
C131—P—C121104.26 (17)C121—C126—H126120.0
C111—P—C121106.13 (17)C136—C131—C132119.3 (4)
C131—P—Pd107.90 (12)C136—C131—P118.6 (3)
C111—P—Pd112.97 (12)C132—C131—P122.1 (3)
C121—P—Pd120.26 (12)C133—C132—C131119.8 (4)
C47—S—C51103.8 (2)C133—C132—H132120.1
C47—S—Pd98.71 (13)C131—C132—H132120.1
C51—S—Pd107.62 (15)C134—C133—C132121.0 (4)
C41—O41—Pd129.4 (3)C134—C133—H133119.5
O42—C41—O41123.4 (4)C132—C133—H133119.5
O42—C41—C42117.3 (4)C133—C134—C135119.2 (4)
O41—C41—C42119.3 (4)C133—C134—H134120.4
C47—C42—C43117.3 (4)C135—C134—H134120.4
C47—C42—C41125.2 (3)C134—C135—C136121.0 (5)
C43—C42—C41117.4 (4)C134—C135—H135119.5
C44—C43—C42122.0 (5)C136—C135—H135119.5
C44—C43—H43119.0C131—C136—C135119.7 (4)
C42—C43—H43119.0C131—C136—H136120.1
C45—C44—C43119.9 (5)C135—C136—H136120.1
C45—C44—H44120.1C61—O61—C64109.8
C43—C44—H44120.1O61—C61—C62106.7
C44—C45—C46120.2 (5)O61—C61—H61A110.4
C44—C45—H45119.9C62—C61—H61A110.4
C46—C45—H45119.9O61—C61—H61B110.4
C45—C46—C47119.7 (4)C62—C61—H61B110.4
C45—C46—H46120.1H61A—C61—H61B108.6
C47—C46—H46120.1C61—C62—C63101.9
C42—C47—C46120.8 (4)C61—C62—H62A111.4
C42—C47—S123.6 (3)C63—C62—H62A111.4
C46—C47—S115.6 (3)C61—C62—H62B111.4
C53—C51—C52111.4 (4)C63—C62—H62B111.4
C53—C51—S109.9 (4)H62A—C62—H62B109.2
C52—C51—S106.4 (3)C64—C63—C62101.9
C53—C51—H51109.7C64—C63—H63A111.4
C52—C51—H51109.7C62—C63—H63A111.4
S—C51—H51109.7C64—C63—H63B111.4
C51—C52—H521109.5C62—C63—H63B111.4
C51—C52—H522109.5H63A—C63—H63B109.3
H521—C52—H522109.5O61—C64—C63106.7
C51—C52—H523109.5O61—C64—H64A110.4
H521—C52—H523109.5C63—C64—H64A110.4
H522—C52—H523109.5O61—C64—H64B110.4
C51—C53—H531109.5C63—C64—H64B110.4
C51—C53—H532109.5H64A—C64—H64B108.6
H531—C53—H532109.5C65—O62—C68109.8
C51—C53—H533109.5O62—C65—C66106.8
H531—C53—H533109.5O62—C65—H65A110.4
H532—C53—H533109.5C66—C65—H65A110.4
C32—C31—C36118.1 (4)O62—C65—H65B110.4
C32—C31—Pd123.7 (3)C66—C65—H65B110.4
C36—C31—Pd118.1 (3)H65A—C65—H65B108.6
C31—C32—C33120.7 (5)C65—C66—C67101.9
C31—C32—H32119.7C65—C66—H66A111.4
C33—C32—H32119.7C67—C66—H66A111.4
C34—C33—C32120.1 (6)C65—C66—H66B111.4
C34—C33—H33119.9C67—C66—H66B111.4
C32—C33—H33119.9H66A—C66—H66B109.3
C33—C34—C35120.1 (5)C68—C67—C66101.9
C33—C34—H34119.9C68—C67—H67A111.4
C35—C34—H34119.9C66—C67—H67A111.4
C34—C35—C36120.2 (6)C68—C67—H67B111.4
C34—C35—H35119.9C66—C67—H67B111.4
C36—C35—H35119.9H67A—C67—H67B109.3
C31—C36—C35120.9 (6)O62—C68—C67106.7
C31—C36—H36119.6O62—C68—H68A110.4
C35—C36—H36119.6C67—C68—H68A110.4
C116—C111—C112118.6 (4)O62—C68—H68B110.4
C116—C111—P117.3 (3)C67—C68—H68B110.4
C112—C111—P123.9 (3)H68A—C68—H68B108.6
C111—C112—C113119.9 (5)C612—O63—C69109.8
C111—C112—H112120.1O63—C69—C610106.8
C113—C112—H112120.1O63—C69—H69A110.4
C114—C113—C112120.8 (5)C610—C69—H69A110.4
C114—C113—H113119.6O63—C69—H69B110.4
C112—C113—H113119.6C610—C69—H69B110.4
C115—C114—C113119.7 (5)H69A—C69—H69B108.6
C115—C114—H114120.1C69—C610—C611101.9
C113—C114—H114120.1C69—C610—H61C111.4
C114—C115—C116120.5 (5)C611—C610—H61C111.4
C114—C115—H115119.7C69—C610—H61D111.4
C116—C115—H115119.7C611—C610—H61D111.4
C111—C116—C115120.5 (4)H61C—C610—H61D109.3
C111—C116—H116119.7C612—C611—C610101.9
C115—C116—H116119.7C612—C611—H61E111.4
C122—C121—C126118.8 (4)C610—C611—H61E111.4
C122—C121—P121.6 (3)C612—C611—H61F111.4
C126—C121—P119.6 (3)C610—C611—H61F111.4
C121—C122—C123121.1 (4)H61E—C611—H61F109.3
C121—C122—H122119.5O63—C612—C611106.7
C123—C122—H122119.5O63—C612—H61G110.4
C124—C123—C122119.2 (5)C611—C612—H61G110.4
C124—C123—H123120.4O63—C612—H61H110.4
C122—C123—H123120.4C611—C612—H61H110.4
C123—C124—C125120.8 (5)H61G—C612—H61H108.6
Pd—O41—C41—O42173.2 (3)C47—C46—C42—C43177.7 (6)
Pd—O41—C41—C426.0 (5)C42—C43—C44—C452.5 (8)
O41—C41—C42—C43141.3 (4)C41—C42—C47—S6.8 (6)
O41—C41—C42—C4741.5 (6)C42—C47—S—C5167.5 (4)
C41—C42—C43—C44177.7 (5)

Experimental details

Crystal data
Chemical formula[Pd(C10H11O2S)(C6H5)(C18H15P)]·C4H8O
Mr713.12
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)9.8574 (6), 10.9503 (6), 16.5057 (10)
α, β, γ (°)100.142 (1), 95.803 (1), 96.244 (1)
V3)1730.2 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.68
Crystal size (mm)0.30 × 0.25 × 0.20
Data collection
DiffractometerSiemens SMART CCD area detector
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.82, 0.87
No. of measured, independent and
observed [I > 2σ(I)] reflections
7829, 5613, 5028
Rint0.017
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.041, 0.097, 1.10
No. of reflections5613
No. of parameters386
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.66, 0.50

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1996), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEX (McArdle, 1995), SHELXL97.

Selected geometric parameters (Å, º) top
Pd—C311.988 (4)Pd—P2.2788 (10)
Pd—O412.098 (3)Pd—S2.3611 (10)
C31—Pd—O41170.24 (14)C31—Pd—S90.71 (11)
C31—Pd—P90.77 (11)O41—Pd—S87.47 (8)
O41—Pd—P92.60 (8)P—Pd—S170.55 (4)
O41—C41—C42—C43141.3 (4)C42—C47—S—C5167.5 (4)
O41—C41—C42—C4741.5 (6)
 

Follow Acta Cryst. C
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds